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Plenarvorträge - DPG-Tagungen

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Dynamik und Statistische Physik Donnerstag<br />

presence of shear flow. Generalizing the approach of [2], ferrofluid droplets<br />

are modeled as deformable and orientable ellipsoids of revolution.<br />

The combined effects of a magnetic field and a shear flow on the orientation<br />

and deformation of the droplets are studied. It is found that the<br />

hydrodynamic drag leads to a flow alignment of the droplet orientation.<br />

Predictions for the alignment angle as a function of the applied field are<br />

presented. Some comparisons to experimental data [3] in the absence of<br />

shear are made.<br />

[1] E. Blums, A. Cebers, M.M. Maiorov, Magnetic Fluids, deGruyter,<br />

Berlin 1997.<br />

[2] P. Ilg and M. Kröger, Phys. Rev. E 66, 021501-1 (2002)<br />

[3] A. Lebedev, A. Engel, K.I. Morozov and H. Bauke, New Journal of<br />

Physics 5, 57.1-57.20 (2003)<br />

DY 46.81 Do 16:00 Poster D<br />

The corkscrew instability in a nematic liquid crystal —<br />

•Alberto de Lozar, Wolfgang Schoepf, Lorenz Kramer, and<br />

Ingo Rehberg — Universitaet Bayreuth<br />

A liquid crystal with slightly positive dielectric anisotropy is investigated<br />

in the planar configuration. This system allows for competition<br />

between electroconvection and the homogeneous Frèedericksz transition,<br />

leading to a rather complicated bifurcation scenario. We report measurements<br />

of a novel instability leading to the ”corkscrew” pattern. This state<br />

is closely connected to the Frèedericksz state as it manifests itself as a regular<br />

modulation along a Frèedericksz domain wall, although its frequency<br />

dependence indicates that electroconvection must play a crucial role. It<br />

can be understood in terms of a pitchfork bifurcation from a straight<br />

domain wall. Quantitative characterization is performed in terms of amplitude,<br />

wavelenght and relaxation time. Its wavelenght is of the order of<br />

the probe thickness, while its ondulation amplitude is an order of magnitude<br />

smaller. The relaxation time is comparable to the one obtained for<br />

electroconvection.<br />

DY 46.82 Do 16:00 Poster D<br />

Magneto-rheological study in inverse magnetic fluids using<br />

polystyrene particles — •Saldivar-Guerrero Ruben 1 , Richte<br />

Reinhard 1 , Rehberg Ingo 1 , and Rodriguez-Fernandez Oliverio<br />

2 — 1 Universitaet Bayreuth, Experimentalphysik V — 2 Centro de<br />

Investigacion en Quimica Aplicada<br />

Ferrofluids are colloidal suspensions of magnetic nanoparticles, which<br />

change their behaviour under control of an external magnetic field. But<br />

when for example, they are mixed with polystyrene particles, they present<br />

another interesting properties. The magneto-rheological fluid (MRF) obtained<br />

in this way, can show a solid-fluid transition by an application<br />

of a moderate magnetic field similar to electro-rehological fluids (ERF)<br />

under a electric field. It excels ERF’s because only moderates currents<br />

instead of high voltages are necessary. We study the rheological influence<br />

of the diameter of the immersed polymer particle in MRF and the relation<br />

between the coupling parameter l and the yield point ty for different<br />

magnetic fields applied. The results show that the rheological properties<br />

are increased when the particle diameter increases in a constant magnetic<br />

field. Also we investigate structure formation in the fluid by video<br />

microscopy when a magnetic field is applied.<br />

DY 46.83 Do 16:00 Poster D<br />

Smectic and crystalline order in colloidal monolayers on periodic<br />

one-dimensional substrate potentials — •Jörg Baumgartl<br />

1 , Matthias Brunner 2 , and Clemens Bechinger 1 — 1 2.<br />

Physikalisches Institut, Universität Stuttgart, Pfaffenwaldring 57, 70550<br />

Stuttgart — 2 Fachbereich Physik, Universität Konstanz, 78457 Konstanz<br />

There is growing interest in the phase behavior of two-dimensional<br />

(2D) colloids in the presence of one-dimensional (1D) periodic substrate<br />

potentials. The phase behavior of such systems is determined by two factors:<br />

(i) the relative orientation between the 2D crystal and the periodic<br />

potential troughs which selects a set of Bragg planes running parallel to<br />

the troughs and (ii) the commensurability ratio p = a ′ /d of the spacing<br />

a ′ between these Bragg planes to the period d of the periodic potential.<br />

So far, only the phase behavior for p = 1 was investigated and the following<br />

phases were observed for increasing (non zero) potential strength:<br />

modulated liquid and light-induced crystal. For other commensurability<br />

ratios additional, more complex phases are predicted.<br />

We investigated experimentally the phase behavior for the case p = 2<br />

with the 1D periodic potential being created by two interfering laser<br />

beams. We observed for the first time the theoretically predicted intermediate<br />

phase between modulated liquid and light-induced crystal which<br />

is termed locked smectic. By analyzing the structure factor and the pair<br />

correlation function, this phase is characterized by liquid-like behavior<br />

along the potential troughs. In contrast to the modulated liquid the ordering<br />

perpendicular to the troughs is similar to the crystalline state,<br />

with particles occupying only each second trough.<br />

DY 46.84 Do 16:00 Poster D<br />

Commensurability effects of colloidal monolayers on hexagonally<br />

patterned substrates — •Stefan Bleil 1 , Matthias Brunner<br />

2 , and Clemens Bechinger 1 — 1 2. Physikalisches Institut, Universität<br />

Stuttgart, Pfaffenwaldring 57, 70550 Stuttgart — 2 Fachbereich<br />

Physik, Universität Konstanz, 78457 Konstanz<br />

Colloidal suspensions are excellent model systems for investigations<br />

of phase transitions in two-dimensional (2D) systems. While most of<br />

the previous work concentrated on homogeneous substrates, much less<br />

is known about the phase behavior on patterned substrates although<br />

the latter closely resembles the behavior of atomic adsorbates on crystalline<br />

surfaces. In our experiments we mimic 2D patterned substrates<br />

for colloidal particles by the interference pattern of several laser beams<br />

which lead to triangular substrate potentials. We present results where<br />

the number density of charge stabilized colloidal particles was systematically<br />

varied. This allowed us to study the effect of the filling fraction<br />

η (i.e. the ratio between the number of colloidal particles and the number<br />

of substrate wells) on the observed structure of the colloidal system.<br />

Depending on the filling fraction we observe commensurate and incommensurate<br />

structures. We also compare our results with recent numerical<br />

simulations.<br />

DY 46.85 Do 16:00 Poster D<br />

Phasetransitions in Quantum fluids: PIMC - Studies — •Guido<br />

Günther and Peter Nielaba — Lehrstuhl für Theoretische Physik,<br />

Fachbereich Physik, Universität Konstanz, D-78457 Konstanz<br />

Exploiting path integral Monte Carlo methods we studied the behavior<br />

of the fluid phase of quantum mechanical hard sphere- and disk- systems.<br />

We focused on the superfluid phase transition of Bose systems<br />

analyzing, among other quantities, the superfluid fraction which in<br />

periodic boundary conditions is related to the winding number of the<br />

Trotter-chains [0].<br />

[0] E.L. Pollock, D.M. Ceperley; Phys. Rev. B 36, 8343 (1987)<br />

DY 46.86 Do 16:00 Poster D<br />

Microcanonical entropy of classical spin systems with a continuous<br />

symmetry — •Andreas Richter, Michel Pleimling,<br />

and Alfred Hüller — Institut für Theoretische Physik I, Universität<br />

Erlangen-Nürnberg, D-91058 Erlangen<br />

Critical phenomena of classical spin systems may be studied in many<br />

ways. In our approach we determine and analyse the microcanonical entropy<br />

S which is related to the density of states by S = kB ln Ω, where kB<br />

is the Boltzmann constant. Due to the huge amount of possible configurations<br />

it is in general impossible to calculate Ω exactly, even for systems<br />

of moderate size. The density of states can, however, be computed approximately<br />

from a numerical method using transition variables. Discrete<br />

classical systems, like the Ising or Potts model, were already studied with<br />

this method in the past [1,2]. We now extend this method to systems with<br />

continuous spins and apply it to the three-dimensional XY model. In addition,<br />

we discuss the determination of critical quantities directly from<br />

the numerically determined microcanonical entropy.<br />

[1] A. Hüller, M. Pleimling, Int. J. Mod. Phys. C 13, 947 (2002)<br />

[2] H. Behringer, J. Phys. A: Math. Gen 36, 8739 (2003)<br />

DY 46.87 Do 16:00 Poster D<br />

A Topological Rule-of-Thumb for Percolation Thresholds —<br />

•Richard Neher and Herbert Wagner — Sektion Physik, Universität<br />

München<br />

Randomly assembled structures exhibit a density driven percolation<br />

transition, beyond which an unbounded component is formed. Since properties<br />

of those structures change dramatically at the percolation threshold,<br />

its accurate knowlegde is important and various empirical formulas,<br />

predicting percolation thresholds, have been suggested. The mean Euler<br />

characteristic is a topological measure for such random sets and it has<br />

been suggested to use its zero crossing to estimate the threshold. In contrast<br />

to other formulas, this estimation does not rely on a fit to known<br />

thresholds.<br />

We further investigated this matter and found, that for a great variety

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